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Optics Express

Optics Express

  • Editor: C. Martijn de Sterke
  • Vol. 20, Iss. 20 — Sep. 24, 2012
  • pp: 21888–21895
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Huge local field enhancement in perfect plasmonic absorbers

M. Albooyeh and C. R. Simovski  »View Author Affiliations


Optics Express, Vol. 20, Issue 20, pp. 21888-21895 (2012)
http://dx.doi.org/10.1364/OE.20.021888


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Abstract

In this work we theoretically reveal the huge local field enhancement in a so-called perfect plasmonic absorber. We study the power absorption of light in a planar grid modelled as an effective sheet with zero optical thickness. The key prerequisite of the total absorption is the simultaneous presence of both resonant electric and magnetic modes in the structure. We show that the needed level of the magnetic mode is achievable using the effect of substrate-induced bianisotropy. On the microscopic level this bianisotropy is a factor which results in the huge local field enhancement at the same wavelength where the maximal absorption holds.

© 2012 OSA

1. Introduction

Total absorption (TA) of light at a certain wavelength in a lossy layer located on a substrate implies simultaneous suppression of both reflection of the incident wave and transmission of this wave into the substrate. This effect has been applied in optical sensing and energy harvesting devices [1

1. C. Luo, A. Narayanaswamy, G. Chen, and J. D. Joannopoulos, “Thermal radiation from photonic crystals: A direct calculation,” Phys. Rev. Lett. 93, 213905 (2004). [CrossRef]

4

4. H. A. Atwater and A. Polman, “Plasmonics for improved photovoltaic devices,” Nature Mat. 9, 205–213 (2010). [CrossRef]

]. However, in the majority known optical absorbers the TA regime is not achievable and can be only more or less approached [5

5. R. M. A. Azzam, E. Bu-Habib, J. Casset, G. Chassaing, and P. Gravier, “Antireflection of an absorbing substrate by an absorbing thin film at normal incidence,” Appl. Opt. 26, 719–722 (1987). [CrossRef]

]. In the microwave and mm wave ranges the TA was engineered exactly in the so-called Dallenbach absorber (see e.g. in [6

6. K. J. Vinoy and R. M. Jha, Radar Absorbing Materials: From Theory to Design and Characterization (Kluwer: Boston, USA, 1999).

]) which comprises a metal substrate. In the optical range the TA was obtained in the so-called coherent perfect absorber using two incident waves [7

7. W. J. Wan, Y. D. Chong, L. Ge, H. Noh, A. D. Stone, and H. Cao, “Time-reversed lasing and interferometric control of absorption,” Science 331, 889–892 (2011). [CrossRef]

]. In both these cases the absorber was a bulk lossy layer and the destructive wave interference in presence of two reflecting boundaries was used. Recently, the TA has been predicted for so-called perfect plasmonic absorbers (PPA) [8

8. N. Liu, M. Mesch, T.s Weiss, M. Hentschel, and H. Giessen, “Infrared perfect absorber and its application as plasmonic sensor,” Nano Lett. 10, 2342–2348 (2010). [CrossRef]

10

10. M. K. Hedayati, M. Javaherirahim, B. Mozooni, R. Abdelaziz, A. Tavassolizadeh, V. S. K. Chakravadhanula, V. Zaporojtchenko, T. Strunkus, F. Faupel, and M. Elbahri, “Design of a perfect black absorber at visible frequencies using plasmonic metamaterials,” Adv. Mat. 23, 5410–5414 (2011). [CrossRef]

]. PPA is a very thin and optically dense planar grid of plasmonic nanoparticles (nanodisks or nanopatches) separated by an optically thin dielectric gap from a metal substrate. Planar grids of resonant particles can be homogenized using the surface averaging of their microscopic responses (see e.g. [11

11. C.L. Holloway, M.A. Mohamed, E.F. Kuester, and A. Dienstfrey, “Reflection and transmission properties of a metafilm: with an application to a controllable surface composed of resonant particles,” IEEE Trans. Electro-magn. Compat. 47, 853–865 (2005). [CrossRef]

, 12

12. C. R. Simovski, “On electromagnetic characterization and homogenization of nanostructured metamaterials,” J. Opt. 13, 013001 (2011). [CrossRef]

]). Such homogenized resonant grids presented as infinitesimally thin sheets of surface polarization were called metasurfaces or metafilms. The mechanism of the TA in known PPAs is still the destructive wave interference. The wave reflected from the metal substrate cancels out with that reflected from the metafilm [9

9. M. Pu, C. Hu, M. Wang, C. Huang, Z. Zhao, C. Wang, Q. Feng, and X. Luo, “Design principles for infrared wide-angle perfect absorber based on plasmonic structure,” Opt. Express 19, 17413–17420 (2011). [CrossRef]

, 10

10. M. K. Hedayati, M. Javaherirahim, B. Mozooni, R. Abdelaziz, A. Tavassolizadeh, V. S. K. Chakravadhanula, V. Zaporojtchenko, T. Strunkus, F. Faupel, and M. Elbahri, “Design of a perfect black absorber at visible frequencies using plasmonic metamaterials,” Adv. Mat. 23, 5410–5414 (2011). [CrossRef]

]. This cancellation becomes possible due to the resonant properties of the plasmonic grid.

In the present paper we suggest a novel type of PPA with another mechanism of the TA and with an additional functionality. In our PPA the transmittance into the substrate is prevented even if the substrate is transparent and the reflectance is prevented in the absence of the second reflecting boundary. The TA is achieved due to the combination of the electric and magnetic modes in the structure. Additionally, our PPAs possess huge local field enhancement (LFE) in strongly subwavelength volumes exactly at the same frequency where TA occurs. The effect of LFE is very important in numerous applications and has been recently widely studied (see e.g. [13

13. S. Kim, J. Jin, Y. J. Kim, I. Y. Park, Y. Kim, and S. W. Kim, “High-harmonic generation by resonant plasmon field enhancement,” Nature 453, 757–760 (2008). [CrossRef]

17

17. B. Rothenhausler and W. Knoll, “Surface plasmon microscopy,” Nature 332, 615–617 (1988).

]). The combination of TA and LFE is very advantageous, e.g. for the surface enhanced Raman scattering (SERS). In many of SERS schemes the LFE holds in a targeted spatial region (e.g. at the nanopatterned surface of silver or gold) and results in the giant enhancement of the Raman radiation from this region [18

18. E. C. Le Ru and P. G. Etchegoin, Principles of Surface-Enhanced Raman Spectroscopy and Related Plasmonic Effects (Elsevier: Oxford, UK, 2009).

, 19

19. K. Kneipp, M. Moskovits, and H. Kneipp, Surface-Enhanced Raman Scattering, Physics and Applications (Eds., Springer: Berlin–Heidelberg–New York, 2006). [CrossRef]

]. Both reflected and transmitted waves are parasitic signals whose presence hinders the detection of the Raman radiation from the targeted spatial region [18

18. E. C. Le Ru and P. G. Etchegoin, Principles of Surface-Enhanced Raman Spectroscopy and Related Plasmonic Effects (Elsevier: Oxford, UK, 2009).

, 19

19. K. Kneipp, M. Moskovits, and H. Kneipp, Surface-Enhanced Raman Scattering, Physics and Applications (Eds., Springer: Berlin–Heidelberg–New York, 2006). [CrossRef]

]. Thus, for prospective SERS schemes it is advantageous to use PPAs (if they possess the LFE effect). While in known PPAs power absorption enhances the local fields (see e.g. [20

20. Y. Chu, Mohamad G. Banaee, and K. B. Crozier, “Double-resonance plasmon substrates for surface-enhanced Raman scattering with enhancement at excitation and stokes frequencies,” ACS Nano 4, 2804–2810 (2010). [CrossRef]

]) these two effects do not take place at the same frequency. However in the present PPA as we show they both occur at the same frequency resulting a purely nonparasitic structure with enhanced field which makes it a proper candidate for optical sensing devices.

2. The key condition for total absorption in a metafilm

First, let us show that it is possible to achieve the TA in a metafilm without any substrate. Consider an optically dense planar array of particles possessing both electric and magnetic polarizabilities and located in free space. Alternatively, we can have in mind one electric dipole and one magnetic dipole per unit cell located in the grid plane. This planar array can be modelled as a metafim with both electric and magnetic surface polarizations [11

11. C.L. Holloway, M.A. Mohamed, E.F. Kuester, and A. Dienstfrey, “Reflection and transmission properties of a metafilm: with an application to a controllable surface composed of resonant particles,” IEEE Trans. Electro-magn. Compat. 47, 853–865 (2005). [CrossRef]

, 12

12. C. R. Simovski, “On electromagnetic characterization and homogenization of nanostructured metamaterials,” J. Opt. 13, 013001 (2011). [CrossRef]

]. Let us show that the TA in the metafilm is achievable with realizable parameters describing its electromagnetic response. For simplicity the array is assumed to be isotropic in the XY-plane and a plane wave impinging normally to the array plane, see Fig. 1(a). Then according to [11

11. C.L. Holloway, M.A. Mohamed, E.F. Kuester, and A. Dienstfrey, “Reflection and transmission properties of a metafilm: with an application to a controllable surface composed of resonant particles,” IEEE Trans. Electro-magn. Compat. 47, 853–865 (2005). [CrossRef]

, 21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

] one can describe the response of the effective sheet by two surface susceptibilities αxxee and αyymm. The relationship between the electric and magnetic surface polarizations and the mean values of the electric and magnetic fields at the grid plane can be written as [11

11. C.L. Holloway, M.A. Mohamed, E.F. Kuester, and A. Dienstfrey, “Reflection and transmission properties of a metafilm: with an application to a controllable surface composed of resonant particles,” IEEE Trans. Electro-magn. Compat. 47, 853–865 (2005). [CrossRef]

, 21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

]:
𝒫x=αxxee<Ex>,y=αyymm<Hy>.
(1)
Here <E> and <H> are defined as the averaged values of electric and magnetic fields taken on two sides of the effective sheet, 𝒫x and ℳy are the electric and magnetic surface polarizations, respectively. Using the boundary conditions for such metafilms derived in [11

11. C.L. Holloway, M.A. Mohamed, E.F. Kuester, and A. Dienstfrey, “Reflection and transmission properties of a metafilm: with an application to a controllable surface composed of resonant particles,” IEEE Trans. Electro-magn. Compat. 47, 853–865 (2005). [CrossRef]

, 21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

], we obtain from Eq. (1):
R=X1+X+Y1+Y,T=1X1+XY1+Y.
(2)
Here R and T are complex reflection and transmission coefficients, respectively, and it is denoted: X=i2k0ε0αxxee, Y=i2k0μ0αyymm, where k0 is the free space wave number (μ0 and ε0 are free space permeability and permittivity, respectively).

Fig. 1 (a) – Horizontally isotropic scatterers with both electric and magnetic responses (e.g. magneto-dielectric spheres experiencing the magnetic and electric Mie resonances at microwaves). (b) – Horizontally isotropic grid of plasmonic particles located over a semiconductor substrate.

Now from Eq. (2) it is easy to see that R = T = 0 if electric and magnetic susceptibilities are, respectively, equal to:
αxxee=2iε0k0,(a),αyymm=2iμ0k0.(b)
(3)

Both required electric and magnetic polarizabilities are purely imaginary that is achievable if the electric and magnetic resonances of our particles coincide. This is definitely a realizable requirement, i.e. the regime when the absorption coefficient A ≡ 1 − |R|2 − |T|2 equals to unity is possible. The key prerequisite for total power absorption is the resonant magnetic susceptibility (Eq. (3-b)) created in addition to the electric one (Eq. (3-a)). This is not problematic at microwaves, however for the visible frequency range becomes challenging. Therefore further we show how to engineer the surface magnetic polarization for a metafilm without any magnetic susceptibility in this range. Moreover we show how to combine the TA together with the LFE obtaining this way a new functionality of PPA layers.

3. Practical solution for simultaneously maximal power absorption together with local field enhancement at optical frequency range

The proposed PPA depicted in Fig. 1(b) comprises an optically dense planar grid (e.g. a square array with the period pλ) of plasmonic nanospheres with the optically small diameter D located over the surface of a strongly refracting half-space at a very small distance s from it.

In previously known PPAs plasmonic nanoparticles were thin tablets and the plasmonic grid formed the effective plane of reflection clearly distinct from a metal interface. Thus, the reflection in previously known PPAs was prevented due to the wave interference [9

9. M. Pu, C. Hu, M. Wang, C. Huang, Z. Zhao, C. Wang, Q. Feng, and X. Luo, “Design principles for infrared wide-angle perfect absorber based on plasmonic structure,” Opt. Express 19, 17413–17420 (2011). [CrossRef]

] whereas the transmittance was prevented due to the total reflectance of the metal substrate. In the present case the distance s between the lower edges of nanospheres and the semiconductor surface is much smaller than D and the geometry does not contain two effective reflection planes. The only reflection plane is the interface to which we refer our metafilm. The resonant magnetic polarization in our metafilm arises due to the so-called substrate-induced bianisotropy which was theoretically revealed and studied in [21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

] for arrays of resonant electric dipoles located on top of a half-space with high refractive index. For the visible range this implies a semiconductor substrate. In plasmon resonance band of silver particles the electric field concentrated within a hot-spot partially located inside the nanoparticle, partially in the substrate. The electric field vectors within the hot-spot have nearly the same phase. However, local polarization currents in the two parts of the hot-spot have opposite directions because the permittivity of the metal is negative and that of the semiconductor substrate is positive. Moreover, the absolute values of these permittivities are comparable to each other. Therefore the polarization of the hot-spot can be presented as a pair of opposite electric dipoles with comparable amplitudes and opposite directions. This phenomenon leads to produce a local magnetic moment which is called electromagnetic polarizability and the effect is named substrate-induced bi-anisotropy since it happens due to the presence of the substrate [21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

]. Here, in our case, both reflection and transmission are prevented due to the balance of the effective electric and magnetic polarizations of a metafilm. However, the most important effect is the regime of LFE, i.e. the new suggested functionality of our PPA. The created magnetic resonance is responsible for the LFE effect [22

22. D. A. Genov, A. K. Sarychev, V. M. Shalaev, and A. Wei, “Resonant field enhancements from metal nanoparticle arrays,” Nano. Lett. 4, 153–158 (2004). [CrossRef]

] and since this resonance mode is the key prerequisite for the TA effect then both effects intrinsically take place at the same frequency.

In this study we consider the normally incident plane wave and a free space gap s. This is done for simplicity and to stress that the wave interference does not play any role. The same functionality can be shown for obliquely incident waves and for nanospheres located on a 1–3 nanometer thick intermediate layer with low refractive index. Although small plasmonic nanospheres possess only the electric dipole response, the presence of the high-contrast substrate leads to the excitation of the magnetic mode [21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

]. This fact is illustrated by Fig. 2(a) which also shows the LFE in the proposed scheme of the PPA. Figure 2(a) is the color map of the field amplitude in the central cross section of a unit cell. This field distribution was simulated at the wavelength λMPA of maximal power absorption (MPA) achievable for this structure (A ≈ 0.99). Dimensions of the structure and parameters of the used materials at λMPA are summarized in Table 1, see also Fig. 1(b). The complex permittivities of Ag and a-Si were taken from [23

23. I. El-Kady, M. M. Sigalas, R. Biswas, K. M. Ho, and C. M. Soukoulis, “Metallic photonic crystals at optical wavelengths,” Phys. Rev. B 62, 15299–15302 (2000). [CrossRef]

] and [24

24. A. S. Ferlauto, G. M. Ferreira, J. M. Pearce, C. R. Wronski, R. W. Collins, X. Deng, and G. Ganguly, “Analytical model for the optical functions of amorphous semiconductors from the near-infrared to ultraviolet: Applications in thin film photovoltaics,” J. Appl. Phys. 92, 2424–2436 (2002). [CrossRef]

], respectively. Since λMPA is within the range of the plasmon resonance of the nanosphere it acquires a large dipole moment. In accordance with the quasi-static image principle calculating the near field one can replace the substrate by an image of the nanosphere. The local field is enhanced mainly in the gap between the nanosphere and the substrate (see Fig. 2(a)). This is similar to the operation of a nanoantenna [14

14. T. H. Taminiau, F. D. Stefani, F. B. Segerink, and N. F. van Hulst, “Optical antennas direct single-molecule emission,” Nat. Photonics 2, 234–237 (2008). [CrossRef]

]. This is not a usual situation since the hot spot in the gap arises for the horizontal polarization of the incident field. However a similar mode has been known for non-symmetric dimers of plasmonic spheres [25

25. V. V. Klimov and D. V. Guzatov, “Strongly localized plasmon oscillations in a cluster of two metallic nanospheres and their influence on spontaneous emission of an atom,” Phys.Rev. B 75, 024303 (2007). [CrossRef]

]. In this dimer the mode analogous to our one is characterized by a strong local polarization of both spheres near their internal edges. In our case the role of the second sphere is played by the image of the first one created by the substrate. To obtain this regime we need a strong optical contrast between two half-spaces and a sufficient curvature of the nanoparticle [26

26. S. A. Maier and H. A. Atwater, “Plasmonics: Localization and guiding of electromagnetic energy in metal/dielectric structures,” J. Appl. Phys. 98, 011101 (2005). [CrossRef]

].

Fig. 2 (a) – Color map of the local field amplitude normalized to that of the incident wave at the wavelength of maximal power absorption. (b) – Coefficients of reflection (amplitude), transmission (amplitude), and absorption (power) of the normally incident plane wave in the proposed plasmonic structure (HFSS vs CST).

Table 1. Dimensions of the PPA and characteristic parameters of materials at the wavelength λMPA=361.9 nm.

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Figure 2(a) also illustrates the substrate-induced bianisotropy. Since the gap s is very small a noticeable part of the hot spot turns out to be located inside the semiconductor. This local polarization of the substrate is concentrated in a nanovolume at a noticeable distance from the effective dipole of the nanosphere. One can check that at λMPA these two effective dipoles (they are both horizontally directed) have opposite phases. The unit cell of the proposed PPA is then equivalent to a pair of electric and magnetic dipoles. Due to the optical smallness of the cell both these dipoles can be referred to the interface. After the homogenization the structure becomes an effective sheet of resonant electric and magnetic surface polarizations. Whereas the LFE in the PPA results from the magnetic mode and the curvature of the nanoparticle, the TA can be explained as we have done above – using the homogenization model.

Using the same model as in [21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

] three effective tangential susceptibilities per unit area of the metafilm can be introduced by relations:
𝒫x=αxxee<Ex>+αxyem<Hy>,y=αyxme<Ex>.
(4)
Here αxyem and αyxme are the electro-magnetic and magneto-electric surface susceptibilities, respectively. Due to the reciprocity we have αxyem=αyxme (see e.g. [27

27. A. Serdyukov, I. Semchenko, S. Tretyakov, and A. Sihvola, Electromagnetics of Bi-anisotropic Materials: Theory and Applications (Gordon and Breach Science: Amsterdam, The Netherlands, 2001).

]), and only two susceptibilities remain in Eq. (4). Using boundary conditions derived in [21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

] we relate the complex reflection and transmission coefficients R and T with these susceptibilities and obtain the retrieval formulas:
αxxee=i4ε0k01R2nT2(1+R+T)2,αxyem=i2ε0μ0k01+RT1+R+T
(5)

The solution corresponding to the total absorption when R = T = 0 and A = 1 is evident:
αxxee=4iε0k0,αxyem=2iε0μ0k0.
(6)

It has been proven in [21

21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

] that for such a structure the surface magnetic polarization is a hundred time smaller than the electric one. Therefore literally we are allowed to neglect such a magnetic polarizability (αmm ≈ 0) in our formalism. Moreover, in the theory of a bianisotropic particle it is shown [27

27. A. Serdyukov, I. Semchenko, S. Tretyakov, and A. Sihvola, Electromagnetics of Bi-anisotropic Materials: Theory and Applications (Gordon and Breach Science: Amsterdam, The Netherlands, 2001).

] that energy is conserved if Im{αee,mm} ≥ 0 and Re{αem,me} ≥ 0 which clearly holds in Eq. (6). Imaginary electric susceptibility in Eq. (6) is achievable exactly and corresponds to the maximum of electric losses in the metafilm. Imaginary magneto-electric susceptibility, on the contrary, corresponds to the absence of magneto-electric losses [27

27. A. Serdyukov, I. Semchenko, S. Tretyakov, and A. Sihvola, Electromagnetics of Bi-anisotropic Materials: Theory and Applications (Gordon and Breach Science: Amsterdam, The Netherlands, 2001).

]. Strictly speaking the TA regime corresponding conditions (Eq. (6)) is an idealization: one can hardly create a metafilm with lossless electro-magnetic (magneto-electric) response. However, one can approach the target conditions in Eq. (6) very closely. We refer to this regime as to that of maximal power absorption.

In our simulations, for a double check, we have used both HFSS and CST software packages with different solution methods. HFSS uses adaptive Finite Element Method (FEM) while CST uses Finite Difference Time Domain (FDTD) method. We have used periodic boundary conditions in order to imitate an infinite array of particles. Taking the benefit of periodic boundary conditions together with the Floquet ports is a well-known method in the analysis of infinite arrays (see e.g. [28

28. J. C. Vardaxoglu, Frequency Selective Surfaces: Theory and Design (Research Studies Press, Ltd.: Taunton, UK, 1997).

]). Reflection, transmission, and absorption coefficients of this PPA versus frequency are calculated using these two packages and are plotted in Fig. 2(b). One can see good agreement between these two different methods (frequency shift of 0.05%). Using simulated reflection and transmission coefficients (amplitudes and phases) and substituting these data into Eq. (5) we have retrieved the corresponding electric and electro-magnetic susceptibilities. The target susceptibilities (Eq. (6)) and those retrieved for the proposed PPA at the wavelength λMPA are presented for comparison in Table 2. For spheres with D = 60 nm over the a-Si substrate this disagreement between ideal and retrieved susceptibilities is minimal over all possible λ and s. It is seen from Table 2 that the energy conservation criteria, i.e. Im{αxxee}0 and Re{αxyem}0 hold obviously. Sensitivity analyses are shown in Fig. 3 to investigate the effect of structure parameters s and D on the maximum absorption level, wavelength, and local field enhancement. The bigger diameters and the smaller gap distances result in larger wavelengths. In Fig. 3(b) the line with circles shows the dependency A(s) calculated for every s at the corresponding λMPA (for s increasing from 1 to 10 nm the wavelength of MPA λMPA decreases from 381 to 358 nm). The resonance of the local field intensity normalized to that of the incident wave calculated at the brightest point of the hot spot is illustrated by the black line without circles in Fig. 3(b) for the optimal height s = 4 nm. The effect of the maximal LFE holds exactly at the same wavelength as that of MPA, i.e. λLFE = λMPA ≈ 362 nm. The same observation refers to other values of s.

Fig. 3 (a) – Color map of the maximum power absorption as a function of particle diameters D and gap thickness s. Notice: Maximum absorption is 99.9% for s = 6nm and D = 75nm. (b) – Black line: the square power of the local electric field amplitude normalized to that of the incident wave versus wavelength for s = 4 nm. The local field is calculated at the center of the gap. Blue line with circles: the absorbtion coefficient in percent as a function of s calculated at wavelengths λMPA(s). (c) – Color map of λMPA variations as a function of particle diameters D and gap thickness s.

Table 2. Desired and achieved surface susceptibilities of the metafilm with s = 4 nm at the wavelength λMPA =361.9 nm.

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4. Conclusion

In this paper we have theoretically demonstrated a possibility of total absorption in an optically dense planar grid of plasmonic nanoparticles over a transparent substrate. We have shown that this absorption does not result from the destructive wave interference as in previously known PPAs. The effect holds due to the balance of the electric and magnetic polarizations whereas the last one results from the substrate-induced bianisotropy. Moreover, this absorption is accompanied by a huge local field enhancement. This new functionality is granted by an effect similar to the LFE in plasmonic nanoantennas. We have checked by numerous simulations that this huge LFE does not hold for arrays of nanotablets, semi-spheres and other particles without curvature of the lower part. We have found that the larger is this curvature the stronger is the LFE. Though in the present paper the gap between the Ag nanospheres and the a-Si substrate is assumed to be filled with free space, this is not critical. Similar results can be obtained for spheres located on a dielectric medium over another semiconductor substrate by optimizing the structure parameters. For instance with particle diameters D = 75nm located over an intermediate SiO2 substrate of thickness s = 12nm best absorption 99.8% is achievable at λMPA = 372.7nm. Local field intensity enhancement (2 – 3) · 103 that we have revealed above is one order larger than that for known SERS structures with transparent substrates [29

29. Y. Chu and K. B. Crozier, “Experimental study of the interaction between localized and propagating surface plasmons,” Opt. Lett. 34, 244–246 (2010). [CrossRef]

].

Acknowledgments

Finally, authors would like to thank Prof. Sergei Tretyakov, Dr. Pavel Belov, and Mr. Javad Hashemi for clarifying and fruitful discussions.

References and links

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7.

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8.

N. Liu, M. Mesch, T.s Weiss, M. Hentschel, and H. Giessen, “Infrared perfect absorber and its application as plasmonic sensor,” Nano Lett. 10, 2342–2348 (2010). [CrossRef]

9.

M. Pu, C. Hu, M. Wang, C. Huang, Z. Zhao, C. Wang, Q. Feng, and X. Luo, “Design principles for infrared wide-angle perfect absorber based on plasmonic structure,” Opt. Express 19, 17413–17420 (2011). [CrossRef]

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M. K. Hedayati, M. Javaherirahim, B. Mozooni, R. Abdelaziz, A. Tavassolizadeh, V. S. K. Chakravadhanula, V. Zaporojtchenko, T. Strunkus, F. Faupel, and M. Elbahri, “Design of a perfect black absorber at visible frequencies using plasmonic metamaterials,” Adv. Mat. 23, 5410–5414 (2011). [CrossRef]

11.

C.L. Holloway, M.A. Mohamed, E.F. Kuester, and A. Dienstfrey, “Reflection and transmission properties of a metafilm: with an application to a controllable surface composed of resonant particles,” IEEE Trans. Electro-magn. Compat. 47, 853–865 (2005). [CrossRef]

12.

C. R. Simovski, “On electromagnetic characterization and homogenization of nanostructured metamaterials,” J. Opt. 13, 013001 (2011). [CrossRef]

13.

S. Kim, J. Jin, Y. J. Kim, I. Y. Park, Y. Kim, and S. W. Kim, “High-harmonic generation by resonant plasmon field enhancement,” Nature 453, 757–760 (2008). [CrossRef]

14.

T. H. Taminiau, F. D. Stefani, F. B. Segerink, and N. F. van Hulst, “Optical antennas direct single-molecule emission,” Nat. Photonics 2, 234–237 (2008). [CrossRef]

15.

K. Watanabe, D. Menzel, N. Nilius, and H. J. Freund, “Photochemistry on metal nanoparticles,” Chem. Rev. 106, 4301–4320 (2006). [CrossRef]

16.

D. G. Grier, “A revolution in optical manipulation,” Nature 424, 810–816 (2003). [CrossRef]

17.

B. Rothenhausler and W. Knoll, “Surface plasmon microscopy,” Nature 332, 615–617 (1988).

18.

E. C. Le Ru and P. G. Etchegoin, Principles of Surface-Enhanced Raman Spectroscopy and Related Plasmonic Effects (Elsevier: Oxford, UK, 2009).

19.

K. Kneipp, M. Moskovits, and H. Kneipp, Surface-Enhanced Raman Scattering, Physics and Applications (Eds., Springer: Berlin–Heidelberg–New York, 2006). [CrossRef]

20.

Y. Chu, Mohamad G. Banaee, and K. B. Crozier, “Double-resonance plasmon substrates for surface-enhanced Raman scattering with enhancement at excitation and stokes frequencies,” ACS Nano 4, 2804–2810 (2010). [CrossRef]

21.

M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt. 13, 105102 (2011). [CrossRef]

22.

D. A. Genov, A. K. Sarychev, V. M. Shalaev, and A. Wei, “Resonant field enhancements from metal nanoparticle arrays,” Nano. Lett. 4, 153–158 (2004). [CrossRef]

23.

I. El-Kady, M. M. Sigalas, R. Biswas, K. M. Ho, and C. M. Soukoulis, “Metallic photonic crystals at optical wavelengths,” Phys. Rev. B 62, 15299–15302 (2000). [CrossRef]

24.

A. S. Ferlauto, G. M. Ferreira, J. M. Pearce, C. R. Wronski, R. W. Collins, X. Deng, and G. Ganguly, “Analytical model for the optical functions of amorphous semiconductors from the near-infrared to ultraviolet: Applications in thin film photovoltaics,” J. Appl. Phys. 92, 2424–2436 (2002). [CrossRef]

25.

V. V. Klimov and D. V. Guzatov, “Strongly localized plasmon oscillations in a cluster of two metallic nanospheres and their influence on spontaneous emission of an atom,” Phys.Rev. B 75, 024303 (2007). [CrossRef]

26.

S. A. Maier and H. A. Atwater, “Plasmonics: Localization and guiding of electromagnetic energy in metal/dielectric structures,” J. Appl. Phys. 98, 011101 (2005). [CrossRef]

27.

A. Serdyukov, I. Semchenko, S. Tretyakov, and A. Sihvola, Electromagnetics of Bi-anisotropic Materials: Theory and Applications (Gordon and Breach Science: Amsterdam, The Netherlands, 2001).

28.

J. C. Vardaxoglu, Frequency Selective Surfaces: Theory and Design (Research Studies Press, Ltd.: Taunton, UK, 1997).

29.

Y. Chu and K. B. Crozier, “Experimental study of the interaction between localized and propagating surface plasmons,” Opt. Lett. 34, 244–246 (2010). [CrossRef]

OCIS Codes
(240.0310) Optics at surfaces : Thin films
(300.1030) Spectroscopy : Absorption
(160.3918) Materials : Metamaterials
(250.5403) Optoelectronics : Plasmonics
(240.6695) Optics at surfaces : Surface-enhanced Raman scattering

ToC Category:
Optics at Surfaces

History
Original Manuscript: July 30, 2012
Revised Manuscript: August 27, 2012
Manuscript Accepted: August 30, 2012
Published: September 10, 2012

Citation
M. Albooyeh and C. R. Simovski, "Huge local field enhancement in perfect plasmonic absorbers," Opt. Express 20, 21888-21895 (2012)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-20-20-21888


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References

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  4. H. A. Atwater and A. Polman, “Plasmonics for improved photovoltaic devices,” Nature Mat.9, 205–213 (2010). [CrossRef]
  5. R. M. A. Azzam, E. Bu-Habib, J. Casset, G. Chassaing, and P. Gravier, “Antireflection of an absorbing substrate by an absorbing thin film at normal incidence,” Appl. Opt.26, 719–722 (1987). [CrossRef]
  6. K. J. Vinoy and R. M. Jha, Radar Absorbing Materials: From Theory to Design and Characterization (Kluwer: Boston, USA, 1999).
  7. W. J. Wan, Y. D. Chong, L. Ge, H. Noh, A. D. Stone, and H. Cao, “Time-reversed lasing and interferometric control of absorption,” Science331, 889–892 (2011). [CrossRef]
  8. N. Liu, M. Mesch, T.s Weiss, M. Hentschel, and H. Giessen, “Infrared perfect absorber and its application as plasmonic sensor,” Nano Lett.10, 2342–2348 (2010). [CrossRef]
  9. M. Pu, C. Hu, M. Wang, C. Huang, Z. Zhao, C. Wang, Q. Feng, and X. Luo, “Design principles for infrared wide-angle perfect absorber based on plasmonic structure,” Opt. Express19, 17413–17420 (2011). [CrossRef]
  10. M. K. Hedayati, M. Javaherirahim, B. Mozooni, R. Abdelaziz, A. Tavassolizadeh, V. S. K. Chakravadhanula, V. Zaporojtchenko, T. Strunkus, F. Faupel, and M. Elbahri, “Design of a perfect black absorber at visible frequencies using plasmonic metamaterials,” Adv. Mat.23, 5410–5414 (2011). [CrossRef]
  11. C.L. Holloway, M.A. Mohamed, E.F. Kuester, and A. Dienstfrey, “Reflection and transmission properties of a metafilm: with an application to a controllable surface composed of resonant particles,” IEEE Trans. Electro-magn. Compat.47, 853–865 (2005). [CrossRef]
  12. C. R. Simovski, “On electromagnetic characterization and homogenization of nanostructured metamaterials,” J. Opt.13, 013001 (2011). [CrossRef]
  13. S. Kim, J. Jin, Y. J. Kim, I. Y. Park, Y. Kim, and S. W. Kim, “High-harmonic generation by resonant plasmon field enhancement,” Nature453, 757–760 (2008). [CrossRef]
  14. T. H. Taminiau, F. D. Stefani, F. B. Segerink, and N. F. van Hulst, “Optical antennas direct single-molecule emission,” Nat. Photonics2, 234–237 (2008). [CrossRef]
  15. K. Watanabe, D. Menzel, N. Nilius, and H. J. Freund, “Photochemistry on metal nanoparticles,” Chem. Rev.106, 4301–4320 (2006). [CrossRef]
  16. D. G. Grier, “A revolution in optical manipulation,” Nature424, 810–816 (2003). [CrossRef]
  17. B. Rothenhausler and W. Knoll, “Surface plasmon microscopy,” Nature332, 615–617 (1988).
  18. E. C. Le Ru and P. G. Etchegoin, Principles of Surface-Enhanced Raman Spectroscopy and Related Plasmonic Effects (Elsevier: Oxford, UK, 2009).
  19. K. Kneipp, M. Moskovits, and H. Kneipp, Surface-Enhanced Raman Scattering, Physics and Applications (Eds., Springer: Berlin–Heidelberg–New York, 2006). [CrossRef]
  20. Y. Chu, Mohamad G. Banaee, and K. B. Crozier, “Double-resonance plasmon substrates for surface-enhanced Raman scattering with enhancement at excitation and stokes frequencies,” ACS Nano4, 2804–2810 (2010). [CrossRef]
  21. M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” J. Opt.13, 105102 (2011). [CrossRef]
  22. D. A. Genov, A. K. Sarychev, V. M. Shalaev, and A. Wei, “Resonant field enhancements from metal nanoparticle arrays,” Nano. Lett.4, 153–158 (2004). [CrossRef]
  23. I. El-Kady, M. M. Sigalas, R. Biswas, K. M. Ho, and C. M. Soukoulis, “Metallic photonic crystals at optical wavelengths,” Phys. Rev. B62, 15299–15302 (2000). [CrossRef]
  24. A. S. Ferlauto, G. M. Ferreira, J. M. Pearce, C. R. Wronski, R. W. Collins, X. Deng, and G. Ganguly, “Analytical model for the optical functions of amorphous semiconductors from the near-infrared to ultraviolet: Applications in thin film photovoltaics,” J. Appl. Phys.92, 2424–2436 (2002). [CrossRef]
  25. V. V. Klimov and D. V. Guzatov, “Strongly localized plasmon oscillations in a cluster of two metallic nanospheres and their influence on spontaneous emission of an atom,” Phys.Rev. B75, 024303 (2007). [CrossRef]
  26. S. A. Maier and H. A. Atwater, “Plasmonics: Localization and guiding of electromagnetic energy in metal/dielectric structures,” J. Appl. Phys.98, 011101 (2005). [CrossRef]
  27. A. Serdyukov, I. Semchenko, S. Tretyakov, and A. Sihvola, Electromagnetics of Bi-anisotropic Materials: Theory and Applications (Gordon and Breach Science: Amsterdam, The Netherlands, 2001).
  28. J. C. Vardaxoglu, Frequency Selective Surfaces: Theory and Design (Research Studies Press, Ltd.: Taunton, UK, 1997).
  29. Y. Chu and K. B. Crozier, “Experimental study of the interaction between localized and propagating surface plasmons,” Opt. Lett.34, 244–246 (2010). [CrossRef]

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